Pulsating circuit and control system



ct 99 w45 P. GLASS 36,6% I

PULSATING CIRCUIT AND CONTROL SYSTEM Filed Deo. 2, 1942 4 sheets-sheet '1 TIME.

lNPUT 1o 14 INVENTOR l2-= n PAUL @Ll-:55 Y y l -t JO. fmf ATTORNEY Oct. 9, 1945. l P GLASS 2,386,677

PULSATING CIRCUIT AND CONTROL SYSTEM Filed Dec. 2, 1942 4 Sheets-Sheet 2 Il Vb t TIME TIME l mvfsNroR. PAUL GLASS Oct. 9,' i945. P. GLASS 2,386,677

PULSATING CIRCUlT AND-CONTROL SYSTEM Filed Dec. 2, 1942 4 Sheets-Sheet 3 717;':'. 7] 5o y 2 e 5: 3-'c 101m @13 T6 ff i vvv" l I lvo W 15 45 25 5o' I' 314,9' I i :X 11' 2' k8' 5 2O' --21 v 1 15 71V7@. 73. 2 19 f 5 Y mil, 5X A@ una Cu c ou o TUBE l TUB 1' CONDUC'IING CONDUCTING L 1 a' C C d' C C e' Ss es 7 377i?. 76. sxiljmmmml njzu'r )f-C LINE;

INVENTOR. *c LINE PAUL GLASS l ATTORNEY oct. 9, 1945. i P, GLASS 4 2,386,677

PULSATING CIRCUIT AND CONTROL SYSTEM A-G LINK INVENTOR PAUL GLASS BY @www ATTORNEY Patented Oct.. 9, 1945 2,336,677A PULSATING CIRCUIT AND coNTRoL SYS TEM A Paul Glass, Chicago, Ill., assignor to Askanla Regulatoii' Company, Chicago, Ill., a corporation of Application December 2, `1942, Serial No. 467,669

13 Claims.

This invention relates to a pulsation circuit employing a gas discharge tube or relay for supplying periodic groups of current pulses to a load device or consumption circuit. The pulsation circuit involves means for varying the number of pulses in each-pulse group and thereby varying the effective value of the loadcurrent. It also involves means for varying the group frequency of the load current, that is, the rate of groups per unit of time. The pulsation circuit provides a convenient means for establishing a current of Figs. 4 and 5 are curves related to Fig. 3, Fig- 4 showing the variations in plate voltage for the electric signals;

variable effective value from elementary current pulses of substantially vconstant and uniform value. The pulsation circuit is especially useful for supplying direct current of variable value from an alternating current circuit.

My invention also relates to control systems employing the pulsation circuit wherein the number of pulses in each group is controlled in response to variations in an input voltage supplied to the pulsation circuit.

One object ofthe control system is to energize the lad with an average current proportional to the amplitude of the applied signal or control voltage.

Another object is to eliminate thel dead zone" oi the gas discharge tube and to render the tube responsive to signal or control voltages o f low magnitude. This is accomplished by supplying to the grid of the tube an A. C. suppressing voltage of fixed amplitude greatly in excess of that required to prevent conduction of the tube when the suppressing voltage is 180 out of phase with the anode voltage, and then shifting the phase of the suppressing voltage so that it leads the anode voltage by slightly less than 180 and is just on the critical point of allowing conduction of the tube. Conduction of the tube is then controlled by supplying the signal or control voltage to the grid circuit with a phase displacement of substantially 90 with respect to the suppressing voltage, thereby causing a shift in phase of the resultant grid voltage in a direction to cause firing of the tube.4V

Examples of my pulsation circuit and control system are shown in the accompanying drawings, in which f Fig. l is a circuit diagram of one form of pulsation circuit:

Figs. 1a andl lb are a modification of the circuit shown in Fig. l;

Fig. 2 is a diagram of voltag/e waves useful for explaining the operation of the various circuits;

Fig. 3 is a diagram showing three groups of current pulses ilowing in the load circuit;

Fig. 11 is a circuit diagram showing a. control system employing the pulsation circuit shown in Fig. 1 and' embodying two vacuum tubes;

Figs. 12 to 17 inclusive ,are diagrams illustrating phase relations between certain voltages in the circuit of Fig. 10;

Figs. 18, 19 and 20 are circuit diagrams illustrating various arrangements for supplying control voltages izo/they circuit of Fig. 10;

Fig. 21 is a diagram of a remote control system illustrating one application of the circuit of Fig. 10; and

Fig. 22 is adiagram illustrating a modication of the circuit of Fig. 10.

Referring to Fig. 1, I is an electron tube of the gasdischarge type having a plate 2, a control grid 3 and a cathode Cathode l-is shown to be of the iilament type, and is energized from the secondary of a transformer 5 whose primary is connected to the A. C. supply line.

In the plate circuit of tube I points 6, l, being connected to the supply line, represent a source of alternating potential, and'8 is a loadkof any desired kind which is to ble-energized bythe device.

Tracing the grid circuit of tube I, grid 3 is connected through a variable resistor 9 to a parallel network comprising resistor I0 and condenser II. Further in the grid circuit are resistory I4 and condenser l5 which connects to the cathode of tube I at point I6.

The points I2, I3 represent the terminals of a source of potential which is derived from the supply line through potentiometer I1 and a phase shifting network I8. This network is shown to consist of a transformer I9 with a center-tapped secondary, an inductance coil 20, and a variable resistor 2l, but any other phase shifting circuit maybe used instead. A voltage divider or potentiometer 22 is connected between plate 2 and cathode 4 of tube I, and its slider 23 connects through a variable resistor 24 to point I3, whereby resistance 24 is connected in shunt to condenrfl through a variable portion ofi-'potentihe time constant of the resistance-condenser network I0, I I is so arranged that it'is short com-v pared with the time constant of the network l comprising condenser I5, variable resistorl 2l, and part of potentiometer 22. The latter resistance is usually small compared with resistance 24. 'I'he capacitance of condenser I5 is large compared with the capacitance of condenser II..

Referring now to Fig. 2, curve a represents the supply voltage as measured at points 6, 'I of the plate circuit. Curve b is the critical grid voltage characteristic of the gas discharge tube. Curve c shows the A. C. grid voltage, as measured at points I2, I3 when the phase shifter' I8 is adjusted for zero phase shift, that is, the grid voltage c is opposite in phase to plate voltage a. If the phase shifter I8 is adjusted for a phase shift angle I the A. C. grid voltage between points I2 and I3 is represented by curve d.

Before describing the operation of the circuit in detail, it may be stated that the device supplies groups of current pulses to the load, as shown in Fig. 3, each group being formed of half-wave current pulses of equal amplitude and having a frequency equal to the frequency of the supply voltage 6-1. During the time interval tI to t2, which is called the on-time (t') current pulses are being delivered to the load, while during the i interval t2 to t3, called olf-time (t) no current flows. The sum of the on-time plus off-time is equal to the group period T, and the reciprocal of T (group period) is the group frequency. Depending on the character of the load, each group of elementary current pulses may be integrated into asingle current pulse flowing during the on-time t as shown by the dotted pulses p in Fig. 3. The average current supplied to the load will be determined by the ratio of the on-time t' to the group period T, and this ratio may be varied between zero and 1. I'he value `of the 1 in this ratio indicates a continuous series of half-wave current pulses 0r an uninterrupted-rectified alterbeginning of each positive half cycle of curve a,

and current ilows through the load for substantially the entire time ofeach positive half cycle.

slider 22.

according to the adjustment of potentiometer 'I'he downwardly sloping portions of curve 5a in Fig. 5 show variations in the voltage across condenser I5 while the condenser is being charged, and the upwardly sloping portions show changes in the condenser voltage during times of discharge. As will be seen from Fig. 5, condenser I5 never becomes completely discharged and it never reaches the iinal potential eo, but when it reaches a negative potential of a value eo", the potential on the grid is sumciently negative to prevent current from flowing in the tube. During the following oil-time the condenser then discharges through resistor. and potentiometer 22 until it has reached a still smaller negative potential eo at the instant t3. At this time the P0- tential on the grid has been reduced to a sutilciently low negative value to permit current to flow in the tube and a new on-time starts, and the cycle is repeated. As a result, the potential of condenser I5 oscillates between the values eo' and eo" as is shown by solid-line curve 5a in Fig. 5.

The second event taking place in the grid circuit during an on-time refers to condenser II. As is well known an ion grid current ows in the grid circuit of a, gas discharge tube if the grid is at a negative potential during conduction. Thus, condenser II is charged with a polarity indicated in Fig. 1 during each on-time. Since the time constant of the network I0, ll is small compared with the time constant of the circuit I5, 24 the nal potential V across condenser II builds up rapidly at the start of every on-time.

and breaks down as rapidly at the end of the during the on-time and until its positive potential has been exceeded by the increase of negative charge on condenser I5.

The total grid potential at the beginning of every positive half-cycle of the supply voltage determines whether or not the tube will conduct current during the following half-cycle. This total grid potential can be obtained with good approximation by adding the combined condenser potentials of condensers II and I5 to the instanv taneous value of the A. C. voltage across points I2,

During the on-time two different events take place in the grid circuit of the tube. The first concerns the condenser I5 which is connected through resistor 24 in parallel to the plate-cathode potential of the tube, assuming for a moment half wave pulses .which charge the condenser I5 with a polarity indicated in Fig. 1. If the ontime is long enough condenser I5 would finally assume the voltage Eo, correspondingto the negative D. c. component of the p1atecathodevo1tage pulses, or a certain smaller value en (Fig. 5) according to the adjustment of the potentiometerv slider 23. Figs. 3, and 5 all have the same scale along 'thetime but Fig. 5 has an enlarged scale of voltage values with respect to the scale I3. 'I'his latter value depends, of course, on the position of potentiometer I1, and on the amount of phase shift applied by the phase shifter Il. If the total grid potential at the beginning of a- -ing conduction during every positive half-cycleA 0f the Oli-time. At the instant t: the total grid' potential has Just become more negative than the of Figs. 3 and 4. In Fig. 5'the dotted horizontal line Eo represents the negative D. C. component of the plate-cathode voltage pulses, while the horizontal line Yeo represents a smaller potential ycritical grid potential and conduction stops.'l Since the influence of condenser Ii suddenly disappears the total grid potential is made still more negative. according to curve 5c. thus preventing any conduction during the following off-time.

It will now be described how it is possible to adjust. within wide limits, the period of operation or the group frequency and also the ratio of ontime to period of operation, or the average load current. Referring to Fig. 6, the influence of the Phase Shift angle shall be considered rst.

The curve 6a in Fig. 6 shows the increasing potential acquired by condenser I during charging. Curves 6b, 6c and 6d represent the decreasing potential on condenser I5 where the charging is stopped at points 2, 5 and 8, respectively. From the description given previously, it will be understood that condenser I5, is charged during the on-time and its voltage continues to rise until the net voltage impressed on the grid of the tube reaches a value corresponding to the critical cutoil value of the tube. The voltage across condenser 5 will therefore increase to a negative value suicient to overcome the positive voltage V of condenser II and also supply any negative component required to x the potential of the grid 3 at the critical value. In Fig. 6, the negative voltage required on condenser I5 to keep the tube from firing for a certain low phase displacement is represented by the voltage Vb, and the voltage V representsthe voltage component of condenser I5 necessary to overcome the positive voltage of condenser II. Accordingly, when the condenser voltage reaches the point 2 the tube will be cut oii and condenser I5 will begin discharging along the curve 6b.

If the phase angle o is increased so that the voltage I2-I3 leads voltage 6-1 by a smaller amount, then voltage I2-I3 will have a greater positive value (or a smaller negative value) at the instant when the tube would normally start, and this situation would require the condenser I5 to -build up a larger negative potential in order to ance 2| in phase shifter I8. Any other form of phase shifting device may be employed for this purpose.

prevent the starting of the tube. For example,

with an increased angle 4, the condenser I 5 would continue to charge until the potential reached a value corresponding to point 5 on curve 6a, then would out oi the tube. This potential would be suiiicient to overcome the positive voltage V on condenser II and also establish a negative component Vc which is required to neutralize the instantaneous value of the voltage I2-I3 at the beginning of the positive pulse of the plate-cathode voltage. For a still greater angle of the instantaneous positive component of the voltage l2-I3 at the start of each cycle would be correspondingly greater, and condenser I5 must build up to a correspondingly higher negative value before the tube will vbe cut oil. For example, fora still greater value of o, the condenser I5 would continue to charge until its voltage reached the point 8 on curve 6a which is suflicient to neutralize the positive voltage V of condenser II and supply the negative component Vd necessary to overcome the positive instantaneous value of the voltage I2-i3 at the beginning of the platecathode voltage pulse.

As shown in Fig. 6, variation of the phase angle also varies the period of operation T, and the minimum value of T occurs for the condition where the ratio t'/T=0.5.

It is further possible to adjust the on-time t alone leaving the value of t" unchanged by shifting tap 23 on potentiometer 22. This is shown with reference to Fig. 7 in which the phase angle is assumed to be adjusted to a certain value which determines eo' and en". By varying the charging voltage of condenser I5, taken oi! the potentiometer 22, different charging characteristics of condenser I5 can be obtained as shown by curves 1a, 1a', 1a". Curve 'Ia' refers toga high, curve la" to a low charging voltage; Since the discharging characteristic c andthe values eo'v and eo remain unchanged with a change of the charging voltage, it is obvious from Fig. 7 that the oir-times teh-ts', te-ta, te"-ta" are the same in all cases. However, the on-times have been changed, tif-t4' being smaller and ts"t4" being larger than t5-t4. Therefore, the on-time alone can be changed by adjustment of the potentiometer slider 23. The on-time decreases, and therefore the value of the load current decreases, with increase in charging voltage applied ample of Fig. 8, the ratio of t'lT remains conangle with respect to the voltage 6l, the on-l time t increases and the olf-time t".decreases 4so that for the condition shown at the points stant while the vperiod of operation T is prolonged. The reverse is true for a reduction of resistor 24. Thus it is possible to keep the average load current constant while varying the group frequency.

The frequency range of the pulse generator can be greatly extended if two further adjustment methods are combined with the ones already described. The rst refersto a change of the variable resistor 9 which iniiuences the grid current. It is obvious that a reduction of grid current can be obtained by increasing the value of resistance 9, and viceversa. Accordingly the potential V across condenser II can be changedwhich determines the working range eo-eo'.

In Fig. 9 curves 9a and 9c are again the charging and discharging characteristics of condenser I5 for a given value of resistor 9, with lines az, a: indicating the limit potentials eo' and eo" of condenser I5. 1f now resistor 9, for instance, is increased the limit lines :ca: will be transferred to the new positions yy. While the charging characteristic 9a remains the same, the new discharging characteristic is shown to be curve 9c', and the new working range is indicated by points 6', 5', 6|. As can be seen from the example of Fig.

9, the period of operation has been decreasedfrom T to T' while maintaining the ratio t'lT -I -plished by adjusting the potentiometer I' The 'principal effect of this voltage change `is again to influence the relative position of. the limit lines :cx in Fig. 9 moving them closer together for a smaller voltage, as indicated by lines W in Fig. 9, and moving them further apart for higher voltages. Increasing the A, C. grid voltage also-tends to shift lines ma: further from the time axis or vice versa. A change of the ad-A justment of potentiometer I1 thus further exrectified A. C. current where the group frequency` and the ratio *t'/T, i. e., the average energy supplied to the load, is variable within wide limits. 'Ihe amplitude of A. C. grid voltage I2-I3 -will depend upon several factors, including the value of lcondenser I5, the time constant of the Vcircuit of condenser I and the charging voltage applied to condenser I5, but in general the maximum value of I2-I3 should greatly exceed the value required to prevent firing of the tube where the voltage is opposite in phase with respectto the anode voltage. In the normal operation of Fig. 1, voltage I2-I3 would be adjusted in phase so that it leads the anode voltage by an angle somewhat less than 180 an'd the voltage applied to the grid at the-beginning of each positive anode pulse is such as to allow ring. of the tube in the absence ofJ a charge on condenser I5, or where the charge on condenser I5 is below a certain value.

From Fig. 6 it will be seen that for a wide range of control of the effective value of load current by shifting the phase of voltage |2I3, the charging circuit for condenser I5 should permit charging of the condenser to a voltage sevadditional grid elements 9', I0', II'.

asador?,

certain phase relations with respect to the supply voltage and to the voltage at terminals I2-I3, as will be described later, then .the -average current supplied to the load will be proportional to the amplitude of the signal voltage, and it is still possible to adjust the group frequency as explained above. Sincethe modiilcation shown in Fig. 10 is an intermediate step between Fig. 1 and Fig. 11, the operation of Fig. 10 will be understood from the following description of Fig. 11.

The circuit as shown in Fig.'11 is similar to the circuit of Fig. 1, and the same reference numerals are used for elements already contained in the earlier iigure. However, the circuit is supplemented by a second gas discharge tube I' with plate 2', grid 3' and cathode 4', and the The load devices 8 and 8', contained in the plate circuits of tubes I and I respectively, are connected through lthe auxiliary load 25 to point 'l of the voltage source. 'I'he signal or control voltage is applied to the input terminals 26, 21 which are connected to the primary of a transformer 28. The secondary of transformer 28 is center-tapped with tap 29 connected to point I2 while the extremities 30 and 30 of the secondary connect to condensers II and |I' respectively. As can be seen from Fig. 11, 4the grid circuits of tubes I and I are made up of a common branch extending from cathode point I6 rvia points I3 and I2 to point 29 while the individual branches extend from-point 29 via point 30 to grid 3, and via point 30' to grid 3i', respectively.

The signal or control voltage applied to input terminals 26, 2l may be derived from any suiteral times as much as the voltage V to which condenser' I I, is charged by the positive ion current. Also, the maximum instantaneous value of voltage I2-I3 should be of the same order of magnitude as the maximum voltage to whichA condenser I5 may be charged.

In one vactual embodiment of Fig. 1, operating on a 60 cycle supply. it was possible to obtain a period of operation T varying from 0.2 to 12 secthe plate circuitexcept during the --negativepulses of the cathode-plate voltage.

In Fig; 1b condenser I5 is charged during the on-time by the voltage drop across impedance Ia in the cathode lead. Element 8a may be a variable resistance or it'may be the load device. In Fig. 11 it may be the auxiliary load 25.

'Ihe circuit of Fis. 1 can be made responsive vto anexternal signal voltage or control-voltage by introducingl the voltage into the input circuit by means of a transformer connected into' the circuit of resistance' III and condenser II as shown in Fig. E10, the remainder cf the circuit being as indicated in Fig. 1.` If the control voltage hasv able potential source as will be described later. 'Ihe signal voltage is of the salme frequency as the supply line frequency, and is variable in amplitude as well as sign. This is made clear by referring to Fig. |12 where curves I and 2 represent two signals of the same sign andof different amplitudes while curves 3 and l show signals of the reverse sign having the same amplitudes as curves I and 2 respectively. `Fig. 13 shows the same relations in vectorial form with the line :rx indicating the direction of the-signal voltage vector. It is an important feature of this circuit that the direction of this vector (control voltage vector) should'be displaced by approximately 90 degrees with respect to the vector of the supply voltage, as will now be described.

In Fig. 14, vector a represents the line voltage, and vector c the potential across points I2, I3 for zero adjustment of phase shifter I8. Considering now the grid circuit of tube I, Fig. 11, the signal voltage with vector e. is impressed as an additional potential at points 29, 30. Accord- *ing to the above statement the direction of vector -ing a comparatively small signal voltage to the input of the circuit, vector c can be shifted in phase by an angle while its amplitude does not change substantially. Thus the same effect is accomplished as was obtained in Fig. 1 by applying a phase shift at the phase shifter Ii, and consequently tube I will conduct current.

Turning now to the grid circuit of tube I', vectors a and c are the same as before but the signal voltage impressed -between points 29 and 30' is now given by vector e.' as shown in Fig. 15.

Thus a phase shift of the same magnitude but in the opposite direction takes place, preventing tube I' from breaking down at the beginning of the positive half-cycles of the line voltage. As a I result, if the signal voltage is of a sign as indicated by vectors es and es' in Figs. 14 and 15, tube I will conduct current and energize load`8 while tube I' does not supply any energy -to its load 8. If now the sign of the signal voltage is reversed the signs of vectors es and es' are reversed as is shown in Figs. 16 and 17. Evidently now tube I' will deliver current while tube I remains non-conducting. It has thus been shown that according to the sign of the signal one or the other tube delivers current to the load asso ciated with it.

The action of the on-and-of control of loadv current need not be explained here since it operates exactly in the manner as wasv described for the pulse generator. However, one difference should be mentioned regarding the Ynecessity of an auxiliary load resistor 25, shown in Fig. 11. Assume fora moment resistor 25 to be zero; then the potentiometer 22 would be directly connected :to the A. C. line, and the voltage across it would contain no D. C. component to charge condenser I5. Take now the normal case with resistor 25 connected as shown in Fig. 11, and assume tube I conducting during an on-time. Then during a positive half-cycle the voltage across potentiometer 22 will be equal to the line voltage minus the voltage drop across resistor 25 while, during a negative half-cycle, the voltage is equal to the line voltage. Now the potentiometer voltage con- I the voltage curve to position f. Then conduction is still safely prevented as Vlong as no signal is applied to the input. Since, according to Fig. l1., the phase shifter I8 is contained in the common branch of the grid circuits, the pre-phase shift refers to both grids alike.

If now a small signal appears across the input, curve f will be further shifted, according toV the sign of the signal, to position e for one tube causing that tube to conduct current, and to position g forthe other tube preventing it from conducting. The introduction of the phase shifter I8 'therefore eliminates the dead zone which freof as outlined in connection with Fig. 1, it is apparent that the ratio t/T, or the average load current, increases with increasing signal amplitude. Measurements show that a direct proportionality between average load current and signal amplitude can be obtained without difficulty. It should be noted that, so far, the phase shifter It had been assumed to be adjusted for zero phase shift. Its function will now be described. In Fig. 2 curve a again shows the line voltage, curve b the critical grid characteristimand curve c the potential across points I2, I3 with phase shifter It adjusted for zero phase shift. Suppose a signal, applied to the input'terminals; causes curve c to be shifted to the right. 'According to the well known laws of gas discharge tubes conduction cannot occur until curvec has reached a position e just touching characteristic b. In other words, the signal has to exceed a certain value before the device starts to energzeone or 'the other load: A "dead zone is present. Itis the object of phase shifter i8 to reduce this dead zone considerably by pre-shifting the `phase of curve c by a denite angle o. The width of the dead zone, and therefore the amount of phase shift necessary to overcome the dead zone is dependent on the amplitude of voltage I2--I3 and increases with the amplitude of this voltage. As shown in Fig. 2 phase shifter I8 in Fig. 11 is assumed to be adjusted for a phase angle po'shiftins quently causes trouble indevices of the described nature. .Resistor 2I, in the example of Fig. ll,v

the signal should be of line frequency. and its vector direction at the input terminals should be displaced by approximately degrees with respect to the vector of the line voltage. In cases where f the signal source itselfxdoes not deliver a signal of the right phase, an additional phase shifting device can be inserted between signal source and input terminals. Also an amplifier may be connected between the signal source and the input of the device, as will be seen in the following examples.

As a first example, a Wheatstone bridge as signal source is shown in Fig. 18. Since the bridge is connected to the A. C. line its output or signal vector will have the same direction as the line voltage vector. introduced which is so adjusted as to displace the vector of the bridge output voltage by approximately 90 degrees. In this example an ampliiier -33 is shown to be inserted between phase shifter 32 and the input terminals 26, 21 of the device. If the bridge 3i is balanced nosignal will be applied to the input, and neither tube will conduct current. If now the bridge is -unbalanced by moving the slider 34 in one or the other direction, a signal of one or the other sign will be applied to the input terminals, and one or the other tube will deliver current to its load. At the same time, the average amourt of load current will be proportional to the deviation of the slider from the balance position. l

In Fig. 19, as a second example, a bridge circuit is shown consisting of four fixed resistors 35, 36, 31, 38, and two variable inductances 39 and 4t.' One variable and one xed inductance may be used instead. The impedance of coils 39, 40 is assumed to be small compared with the resistance values of resistors 35 and 36. Assuming that the resistance balance condition is fullled an output voltage will appear at points 4I. d2 when the inductance balance is disturbed. In the circuitof Fig. 19 the 'bridge output vector will then be displaced by 90 degreesagainst the supply voltage vector, as follows from the theory of A. C. bridge circuits. In this case no additional phase shifter is required, and the signal voltage is applied to input terminals 26, 21 through amplifier 33, as shown in Fig. 19.

As a third example, in Fig. 20 a pair of selfsynchronous motors is shown as the source of signal potential. Rotor 43 of the transmitter is connected to the A. C. line, and the stators u and 45 are connected in the usual manner. Rotor 46 of the receiver is connected through phase shifter 32 to the input terminals 26, 21. If de- 'I'herefore la phase shifter 32 is out of its balance position in one or the other direction of rotation a voltage will be induced in assaew rotor 46 which is of one'or the other sign according to the direction of original displacement. The direction of the voltage vector of receiver rotor 40 coincides with the direction of the line voltage vector. Therefore, a phase shift of ap; proximately 90 degrees is introduced by phase shifter 22 to obtain the desired phase, relation of the signal voltage. One or the other load will be energized according to the direction of displacement of rotor 43, and the average load current will be proportional to the magnitude of the displacement. It should be mentioned that the wound rotor type ci' self-synchronous motors is preferred although the salient pole type gives also very satisfactory results.

Regarding the load devices 8 and 8', any device may be used' as for instance heaters, relays or solenoids. Another example is a motor of, the series commutator type as load device. In this case, referring to Fig. 11,load 25 represents the motor armature, and l and 8' are two field coils in series with the armature such that energization of one or the other field coil causes the motor to rotate in one or the other direction ofrotation. W'hile the operation of the motor from the pulse control circuit will be understood without further discussion one important point has yet to be mentioned. It has been observed that after correct adjustment of the phase shifter i8 and upon application of small signalsboth tubes became conductive at the same time resulting in a reduction of motor speed and torque. Thus, below a certain small signal voltage the device did not operate satisfactorily. It was possible to eliminate this dead zoneby connecting a condenser C across the plates 2 and 2 of the tubes, as shown in Fig. 11. As an explanation it is believed that a component of.' high frequency and high voltage is superimposed upon the line voltage resulting from the action of th motor commutator. The voltage peaks applied to the plate of the non-conducting tube cause that tube to break down as well. Condenser C, if connected as shown, acts as a short circuit for the high frequency component, and prevents the disturbance from reaching the plate of the non-conducting tube.

A useful combination of signal source and load device with thef pulsation circuit is obtained if a pair of self-synchronous motors is used together with a reversible motor, as described above. In the block diagram of Fig. 2l El is the pulse control circuit of Fig., 1l with the'input terminals 2l, 21.-

The circuit supplies energy to the double field series motor Il as was explained earlier. Coupled to its shaft through a gear train Il is the shaft of a self-synchronous motor l2 whose rotor is electrically connected to the A. C. line. A load l0 may be connected to the shaft of motor I2. Another self-synchronous motor is shown at whose stator is connected in the usual manner to the stator of motor i2, and whose rotor terminals 51 connect through a combined phase shifterand amplifier 54 to the input terminals 2|, 21 of the pulse control circuit.

Assuming that the rotors of motors l2 and I3 V are in the neutral position, no signal voltage is. applied to input terminals 28, 21, and consequently the pulse control circuit does not supply any energy to motor l I. If now the rotor of motor. is displaced in one direction of rotation, a signal is supplied to the input V2O, 21 and circuit 50 causes the motor 5I to rotate in one direction of rotation.' At the same time, the rotor of self-synchronous motor 52 is rotated also, and its direction of rotation is assumed to be such as to reduce the relative displacement of rotors l2 and B3. Consequently the signal at terminals 20, 21 will' be reduced, and so is the motor speed, until motor I2 has reached a new balance position, resulting in signal voltage zero and standstill of motor 5I. As a result, rotor l2 assumes the same angular'position as rotor 53. It is to be noted that the self-synchronous motors are required to furnish only a signal voltage as an indication of their relative rotor positions, but do not transmit anyv 'mechanical torque. 'I'he necessary energy for rotation. of rotor 52 and load l0 into the syn-` chronous position is supplied from the pulse control circuit, and is limited only by the size of the tubes and motor used. Therefore, at the receiving end, i. e., load Il, a high torque with a high accuracy is available while at the transmitting end, i.- e., s haft 53, a very low torque is required for positioning of the transmitting rotor. 'Ihe pulse control circuit in combination with the reversible motor acts as torque amplifier for a set of self-synchronous motors.

In Fig. 22, I have shown a modincation of the circuit of Fig. 11 omitting the pulsating feature.

-In this arrangement, elements corresponding to omits the condenser il and its charging circuit,

and it also omits condensers I i and resistances il. The circuit does include transformer Il and phase shifter Il forfsupplyingth 'suppressing voltage to the grid circuits across terminals i2-i2. As in Fig. l1, the voltage I2-Il has a value greatly in excess of that necessary to prevent operation of the tubes when the suppressing voltage is opposite in phase to the anode voltage, and it is shifted in Phase by phase shifter il to overcome the dead zone" referred to above and to nx th circuit at the critical operating point. The sigial or control voltage supplied to the input terminals 26, 21 may be derived from any suitable source such as from a Wheatstone bridge 3| having a slider I4; the signal voltage being supplied through a phase shifter I2 and an amplifier Il. As explained before, the signal voltage at terminals 20 and 21 has a phase angle of substantially degrees with respect to the anode voltage of the tubes.

A signal voltage of o'ne sign in Fig. 22 will cause l one Ytube toilre and therefore `rotate armature 25 in one direction. while the signal voltage of the oppositesign will cause the other tube to fire and rotate amature 2l in the opposite direction. In .this case, the control of the 'motor circuit will be a simple on-and-oii' control, and the motor operating current will not vary inaccordance with the amplitude of the signal voltage. One advantage of the arrangement of Pig. 22 is that very small signal voltages are required to operate the motor in one direction or the other. In-an actual embodiment, the motor responds to the movement of a magnetic amature of less than :0.001 inch. Another advantage of the control circuit of Fig. 22 is t the action of the circuit is ot material aifected by unavoidable extrane us variati in the amplitude of the control voltage i2- il. 'I'his improved result is obtainedby reason of the fact that in both Figs. 11 and 22, the signal voltage is utilized to control the firing of the tubes by shifting of the phase of the resultant grid voltage instead of by varying the amplitude of the resultant grid voltage as in prior devices.

The time constant of the charging and discharging circuit of condenser I should be adjustable to be relatively long by comparison with the cycle period of the A. C. current supply, that is it should require several cycles to charge or discharge condenser I5.

The circuit of Fig. 1 is useful for any purpose where it is desired to supply a load circuitor device with a current formed of a series of integrated current pulses of variable pulse frequency. and variable ratio of on-time to olf-time. It will be useful in many applications requiring the periodic suppression of current pulses in certain l cycles of an alternating current supply.

Fig. shows how the circuit of Fig. 1 may be used as a control circuit responsive to a variable input signal or control wave. 4that the circuit of Fig. 1 may also be used as a control circuit by merely arranging for one or more of the variable elements of the circuit to bemech'anically varied in accordance with variations in a condition tobe controlled, indicated orrepeated.

What is claimed is:

1. In combination, a, gaseous discharge tube, a grid circuit for said tube including two series connected condensers, an anode circuit for said tube including a source of alternating current, a discharge path connected in shunt to each of said condensers, meansior charging one of said condensers from said anode circuit in a direction to apply a negative potential to said grid, means for supplying an alternating current voltage wave to said grid circuit of the same frequency as said.y source, said alternating grid Voltage wave serv` ing to charge the other condenser in the opposite direction by the positive ion current flowing in said grid circuit during conduction of said tube and having an effective value greatly in excess of the value required to prevent i'lring of said tube when said wave is opposite in phase to the anode voltage wave, and means for variably shift- '6. A combination according to claim 11 wherein said phase shifting means is set to fix the phase of said grid voltage wave to lead the anode voltage wave byan angle slightly less than'V 180 and cuit a control voltage wave'of variable-ampli It will be obvious `cluding means for introducing into saidgrid normally prevents the firing of said tube, and inicircuits in a direction to apply a negative potential to the-grid of each tube, means for supplying from said alternating current source to said grid circuits a. grid voltage wave having an eiective value greatly in excess of the value required to preventing rst of said tubes when said grid waves are opposite in phase to said anode voltage waves, phase shifting means for setting the phase of said grid voltage waveslto a leading angle 4@ said grid circuit an 'alternating voltage wave ing the phase of said grid voltage Wave to thereby vary the effective value of the current in said anode circuit.

2. A combination according to claim 1 wherein the discharge path of the condenser which is charged from the anode circuit has a time constant relatively long with respect to the time constant of the discharge path of the other'series connected condenser.

3. A combination according to claim 1 and including means for varying the charging voltage applied to said one condenser from said anode circuit.

4. A combination according to claim 1 wherein the condenser receiving a charge from the anode circuit is charged to a relatively high value and the other condenser is charged to a relatively` small value by the positive ion current ilowin'g Ain said grid circuit during conduction of said tube.

5. A combination according to claim 1 wherein slightly less than 180 with respect to said anode voltage waves, whereby the dead zone in the control of said tubes is overcome while still suppressing the iring thereof, and'means for introducing into said grid circuits control voltage waves of variable amplitude but of opposite phase relation and being displaced. in phase by substantially with respect to said anode voltage Waves.

8. In combination, a gaseous discharge tube, a

y grid circuit for said tube, an anode circuit for said tube including a source of alternating current, means for .supplying from said source to having an effective value greatly in excess of the value required to prevent firing of said tube when said wave is opposite in phase to the anode voltage wave, phase shifting means for ilxing the phase of said grid voltage wave at a leading angle slightly less than with respect to the anode voltage wave to overcome the dead zone in vthe control ofsaid tube, and means for supply- Ving to said grizi` circuit a control voltage Wave of variable amplitude andI having a leading phase 'angle of substantially 90 with respect to said anode voltage wave.

9. A combination according to claim 8 wherein said control voltage wave varies in amplitude and also reverses in phase, and including a second gaseous discharge tube having a grid circuit supplied with a grid voltage wave from said phase shifting device and a plate circuit supplied from said source, and including means for introducing in the grid circuit of said second tube a control voltage wave from the same source as the control voltage wave introduced in the grid circuit of said rst tube but of opposite phase relation, whereby variations in amplitude ofv said con- 4trol voltage waves increase the phase angle of the resultant Wavein one grid circuit and decrease the' for charging said condenser by the voltage drop across said impedance element, said connection having a relatively long time constant, a second condenser connected in series with said gridcircuit, means for supplying alternating current to said grid circuit to charge said second condenser in the opposite direction by positive ion current, and a discharge path of relatively short time constant connected in shunt to said second condenser.

ll. A combination according to claim 1 wherein said means for charging one of said condensers from said anode circuit comprises an impedance element connected in the cathode lead of said anode circuit, and a connection for charging said one condenser by the voltage drop across said impedance element. l

12. In combination, a gaseous discharge tube, a grid circuit for said tube, an anode circuit for said tube including a source of alternating current, means for supplying from said source to said grid circuit a rbiasing alternating current voltage wave substantially opposite in phase to the anode voltage wave and having an eective I value sumcient normally to prevent iii-ing ot said tube, and means for supplying to said grid cli'- cuit a control voltage wave ofvariable effective amplitude and having a-leading phase angle of substantially 90 with respect to said anode voltage wave.

13. In combination, a pair of gaseous discharge tubes, a-grid circuit for each of said tubes. anode circuits for said tubes including a source of alternating current for supplying anode voltages ot the same phase relation, means for supplying from said -source to said grid circuits altemating voltage waves substantially opposite in phase with respect to the anode voltage waves and havving effective values suillcient normally to pre- PAUL GLASS. 

